Transparent conductors comprising gallium-indium-oxide

Abstract

 Applicant has discovered that aliovalently doped gallium-indium-oxide (GaInO₃) can achieve electrical conductivity comparable to wide band-gap semiconductors presently in use while exhibiting enhanced transparency and improved index matching. The material can be doped to resistivity of less than 10 milliohm-cm by small quantities of aliovalent dopants, such as tetravalent atoms. It has a refractive index of about 1.6 and can be deposited on glass substrates in polycrystalline films.

Description

Field of the Invention

[0001] This invention relates to conducting materials and, in particular, to conducting materials comprising gallium-indium-oxide, GaInO₃, doped to exhibit electrical conductivity in a transparent state.

Background of the Invention

[0002] Only a handful of materials provide the highly useful combination of electrical conduction and optical transparency. The earliest used materials were thin films of gold, silver and platinum used as electrodes on photoelectric cells. Wide band-gap semiconductor transparent electrodes including tin oxide coatings came into use during World War II (Nesa glass), and indium oxide coatings became commercially available in the 1970's. See G. Haacke, "Transparent Conducting Coatings", 7 Ann. Rev. Mater. Sci. 73-93 (1977).

[0003] Transparent conductive materials are important components in visual communications devices and useful in a variety of other applications. In modern liquid crystal displays, for example, arrays of transparent electrodes define the display segments or even pixels to be activated. Moreover transparent conductors can be used as antistatic coatings on instrument panels, heating elements on aircraft windows, and electrodes on solar cells. Such materials are also useful as heat retaining and ultraviolet light-rejecting coatings on windows.

[0004] One difficulty with presently available transparent conductive materials is their narrow transmission spectrum. They tend to absorb blue light in the visible spectrum and some tend even to absorb red light. For example, indium tin oxide, widely used because of its high conductivity, tends to absorb blue light and, as a consequence, appears yellow or green. Similar coloration is observed in a variety of wide band-gap semiconductor materials including zinc indium oxide and cadmium tin oxide. Such absorption requires higher power levels, limits choice in coloration, and presents an impediment to the development of full color flat panel displays. A second difficulty arises from the poor index of refraction match between indium tin oxide (ITO) (the most commonly used transparent conductor) and typical glasses. ITO coatings typically have an index of about 2.0 whereas typical glasses have an index of about 1.5. The result is reflection loss at the ITO/glass interface, reducing the amount of transmitted light. Accordingly, there is a need for transparent conductive material having enhanced transparency and better index matching with glass.

Summary of the Invention

[0005] Applicant has discovered that aliovalently doped gallium-indium-oxide (GaInO₃) can achieve electrical conductivity comparable to wide band-gap semiconductors presently in use while exhibiting enhanced transparency and improved index matching. The material can be doped to resistivity of less than 10 milliohm-cm by small quantities of aliovalent dopants, such as tetravalent atoms. It has a refractive index of about 1.6 and can be deposited on glass substrates in polycrystalline films.

Brief Description of the Drawings

[0006] In the drawings:

FIG. 1 is a polyhedral representation of GaInO₃;

FIG. 2 is a schematic cross section of a substrate coated with conductively doped GaInO₃; and

FIG. 3 is a graphical display of absorption versus wavelength for conductively doped GaInO₃ in comparison with conventional ITO.

Detailed Description

A. Conductively Doped GaInO₃

[0007] Applicant has found that the conductivity of GaInO₃ is enhanced by small quantities of aliovalent dopants M in GaIn_1-xM_xO₃. (An aliovalent dopant is a dopant which has a valence different from the other atoms in the host compound). The aliovalent dopant should have a valence greater than 3 and preferably is tetravalent. In a series of experiments using GaIn_1-xSn_xO₃ with 0.005 ≦ x ≦ 0.12, it was determined that GaIn_0.94Sn_0.06O₃, for example, provided resistivity of 2 milliohm-cm in a 0.6 micrometer thick film. And, a similar series of experiments showed Ga_1-xGe_xInO₃, 0.005 ≦ x ≦ 0.12, to exhibit conductivity equivalent to GaIn_1-xSn_xO₃ and visually similar transparency. GaIn_1-xGe_xO₃ also gives good transparency and conductivity. Doping with Ti or Nb provided enhanced conductivity, but it was two orders of magnitude lower than the conductivity produced by tin. Doping with Si yielded similar results when Si was substituted for Ga. A series of experiments with Ga_1+xIn_1-x-ySn_yO₃ and Ga_1+x-yGe_yIn_1-xO₃ for 0.25 ≧ x and .005 ≦ y ≦ .12 also showed conductivity and good transparency.

[0008] FIG. 1 is a polyhedral representation of the crystal structure of GaInO₃. The metal atoms are in the centers of the polyhedra, and the oxygen atoms are at the corners. The tetrahedra 20 represent GaO₄ and the octahedra 21 represent InO₆.

[0009] GaInO₃ exhibits a β gallia crystal structure similar to one of the forms of Ga₂O₃. In the Ga₂O₃ analog, Ga is present in two crystallographic metal sites: a four coordinate site and a six coordinate site. In GaInO₃, Ga is on the four coordinate site, and In is on the six coordinate site. As a consequence of this similarity, GaInO₃ can be mixed with Ga₂O₃ in a continuous range. GaInO₃ is conductively doped if it is doped to a resistivity of 10 milliohm-cm or less.

[0010] Methods for preparing conductively doped GaInO₃ can be understood by consideration of the following examples.

Example 1

[0011] Powdered gallium oxide, Ga₂O₃, indium oxide, In₂O₃, and tin oxide, SnO₂, are weighed out to yield the appropriate mole ratios for GaIn_1-xSn_xO₃. For instance, for a 5-gram total weight sample of GaIn_.94Sn_.06O₃, 2.0090 grams of Ga₂O₃, 2.7972 grams of In₂O₃ and 0.1938 grams of SnO₂ are used. The powders are mixed together and ground together in a mechanical mortar and pestle for a minimum of five minutes to insure good mixing and contact of powder particles. The mixed powders are transferred into high density aluminum oxide crucibles with cover and heated in air for an initial period of 12-15 hours at temperatures between 1100 and 1200°C. The resulting powders are then ground mechanically again, re-introduced into the covered aluminum oxide crucibles, and heated for a period of 12-15 hours at 1300°C in air. After a third grinding, pellets are pressed in a standard steel dye (typically to a load of 3000 pounds for a half-inch diameter pellet). The pellets are then heated again at 1300°C in air for a period of up to 60 hours. Pellets are typically placed on powder of their own composition inside the covered aluminum oxide crucibles for the pellet firing step. The pellets are cooled after this heating step at the natural cooling rate of the furnace, which in our case results in reaching 300°C in approximately three hours, at which point the pellets are removed from the furnace. The resulting pellets are typically single phase materials (to the detectability limits of standard powder x-ray diffraction) of the GaInO₃ structure type. Air is selected as an ambient for the initial processing steps because of its convenience. Covers are placed over the crucibles as a precaution to prevent evaporation of the oxides, but we have not observed evaporation under the conditions described. The first air firing need not necessarily be in the 1100-1200°C range, but we select an initial low temperature to reduce the possibility of metastable melting. The final heating temperature of 1300°C in air gave more satisfactory conductivities, in one set of experiments, than did a 1400°C air treatment. The times and temperatures of these treatments are expected to be dependent on the reactivities of the starting materials and the efficiencies of the grinding operations. Shorter times can be expected to give equally satisfactory results, for example, in the preparation of ceramic targets for sputtering or laser ablation.

[0012] The material after air firings are not in their optimally conducting state. A further treatment is advantageous to improve the conductivity. In this treatment, a heating of duration 10-12 hours in flowing N₂ (approximately 100 cc/min, N₂ typically approximately 50-100 ppm O₂) in a ceramic tube furnace at 1200°C is employed, again with the pellets allowed to cool at the natural furnace cooling rate. Covered aluminum oxide crucibles and a powder bed for the pellets need not necessarily be employed for this step. The pellets emerge from the N₂ treatment with good electrical conductivity and a light grey-to-white color.

Example 2

[0013] Processing conditions as described in Example 1, with Ga₂O₃,GeO₂, and In₂O₃ mixed in appropriate mole ratios to yield Ga_1-xGe_xInO₃. For example for Ga_.92Ge_.08InO₃ in a 5 gram batch, 1.8470 grams of Ga₂O₃, 0.1792 grams of GeO₂ and 2.9737 grams of In₂O₃ are employed.

Example 3

[0014] Processing conditions as described in Example 1, with Ga₂O₃,In₂O₃ and SnO₂ mixed in appropriate mole ratios to yield Ga_1-xSn_xInO₃. For example, for Ga_.96Sn_.04InO₃ in a 5 gram batch, 1.9158 grams of Ga₂O₃, 0.1283 grams of SnO₂ and 2.9559 grams of In₂O₃ are employed.

Example 4

[0015] Processing conditions as described in Example 1, with Ga₂O₃,In₂O₃ and TiO₂ (titanium dioxide) mixed in appropriate mole ratios to yield GaIn_1-xTi_xO₃. For example for GaIn_.96Ti_.04O₃ in a 5 gram batch, 2.0358 grams of Ga₂O₃, 0.0694 grams of TiO₂, and 2.8948 grams of In₂O₃ are employed.

Example 5

[0016] Processing conditions as described in Example 1, with Ga₂O₃,In₂O₃ and SiO₂ (silicon dioxide) mixed in appropriate mole ratios to yield Ga_1-xSi_xInO₃.

Example 6

[0017] Processing conditions as described in Example 1, with Ga₂O₃,In₂O₃,GeO₂ and SnO₂ mixed in appropriate mole ratios to yield Ga_1-xGe_xIn_1-ySn_yO₃.

Example 7

[0018] Processing conditions as described in Example 1 except that after firing the pellets are heated in a nitrogen-hydrogen (15 mole percent hydrogen) ambient rather than in N₂, and at a temperature of 600-650°C rather than 1200°C. This process produced conductivity of 2 milliohm cm, the highest thus far observed in bulk doped GaInO₃.

Example 8

[0019] Alternatively, for applications which do not require the highest conductivity, pellets of undoped GaInO₃ after firing can be heated in a reducing ambient (e.g. nitrogen-hydrogen (15 mole percent hydrogen) at 600-650°C). Such targets produce conductive films. It is believed that they are effectively doped by oxygen vacancies.

B. Substrates Coated With Conductively Doped GaInO₃

[0020] It is contemplated that a basic use of conductively doped GaInO₃ is providing transparent coatings on substrates such as glass, semiconductor or plastic. For example, the ability of the material to transmit light of any wavelength from 0.4µm to 1.1µm makes it useful as a coating material for windows, solar cells or display devices. Such coated substrates permit selective entry of visible light while reflecting ultraviolet and infrared. FIG. 2 is a schematic cross section of a substrate 30, such as a transparent glass, coated with a thin layer 31 comprising conductively doped GaInO₃. Preferably the coating is in the form of a thin continuous polycrystalline layer having a thickness typically in the range 0.1µm to 1µm.

[0021] The method for coating a substrate 30 can be understood by considering the following examples.

Example 9 (Deposition By Laser Ablation)

[0022] A pressed pellet of Ga_0.9Ge_0.1InO₃ was placed in the target holder of a pulsed laser deposition vacuum chamber and a vitreous quartz substrate was mounted onto a heatable substrate holder facing the target and positioned about 8 cm from the target. The chamber was evacuated to a base pressure of 1-10x10⁻⁷ Torr and 1 m Torr of oxygen was bled into the chamber. The substrate was heated to 250°C, and then the target was bombarded by pulses from a KrF excimer laser operating at 248 nm with a pulse repetition rate at 10 Hz. The energy density of the laser on target was 1-4 J/cm². The deposition rate was 1000-1500 angstroms per hour. After growth of several thousand angstroms, the chamber was again evacuated and the substrate was permitted to cool to room temperature. The films subsequently removed from the chamber were transparent to the eye with good electrical conductivity.

Example 10 (Deposition By Sputtering)

[0023] A pressed pellet of Ga_1-xSn_xInO₃ was placed in the target holder of a dc magnetron sputter deposition chamber. Coming glass and fused silica substrates were placed in proximity to the target in two configurations: (1) on-axis geometry directly underneath the target and (2) off-axis geometry outside the plasma plume, approximately 0.5-2.0 cm from the edge of the sputtering gun. The chamber was evacuated, and a sputtering gas consisting of an argon-oxygen mixture (15-1 ratio) at 4-20 m Torr was introduced. The substrate was heated to 250°C - 500°C. The target was then impacted by the sputter gun (a US 1'' magnetron source) operating at a dc voltage of 350V, a current of 0.78A, and a power level of 25 Watts. The growth rate was about 1.3 µm per hour in the on-axis geometry and .25 to 0.5 µm per hour in the off-axis geometry. The films had resistivity of about 2.5 milliohm-cm in a 0.4 micrometer thick film and exhibited transmission superior to indium tin oxide in the green and blue regions.

[0024] FIG. 3 is a graphical illustration of the absorption spectrum of conductively doped GaTnO₃ (curve 1) in comparison with that of conventional ITO (curve 2). As can be seen, the GaInO₃ film exhibits uniformly small absorption across the visible spectrum.

Claims

1. A transparent conductive material comprising GaInO₃.

2. A transparent conductive material comprising GaInO₃ doped with an aliovalent material having a valence greater than 3.

3. The composition of matter comprising GaInO₃ doped to a resistivity less than 10 milliohm-cm with an aliovalent material having a valence greater than 3.

4. The composition of matter comprising GaIn_1-xM_xO₃ where M is an aliovalent material having a valence greater than 3 and 0.005 ≦ x ≦ 0.12.

5. The composition of matter comprising Ga_1-xM_xInO₃ where M is an aliovalent material having a valence greater than 3 and 0.005 ≦ x ≦ 0.12.

6. The composition of claim 3 or 4 or 5 wherein said aliovalent material is a tetravalent material.

7. The transparent conductive material of claim 2 wherein said aliovalent material is a tetravalent material.

8. The composition of matter comprising Ga_1-xM_xIn_1-xM

O₃ where M and M' are aliovalent materials having valences greater than 3.

9. The composition of claim 8 where M is Ge and M' is Sn.

10. The composition of matter comprising Ga_1+xIn_1-x-yM_yO₃ where M is an aliovalent material having a valence greater than 3, 0.25 ≧ x and 0.005 ≦ y ≦ 0.12.

11. The composition of matter comprising Ga_1+x-yM_yIn_1-xO₃ where M is an aliovalent material having a valence greater than 3, 0.25 ≧ x and 0.005 ≦ y ≦ 0.12.

12. The composition of claim 2 or 3 or 4 or 5 or 7 or 8 or 10 or 11 wherein the dopant material comprises a material from the group consisting of tin, germanium, silicon, niobium and titanium.

Drawing